Let me do the simple calc ignoring black hole creation business and go with ideal gas assumptions:
The initial volume is the volume of heart: V
i = 1.08321*10^21 m^3 (according to google)
The initial heat to use is more debatable. For the sake of a low end let's use average global surface temperature: T = 14°C = 287.15K
For the initial pressure let's use: P
i = 1 atm = 101325 Pa = 101.325 kPa
R = 8.31446261815324 J/(K * mol) be the ideal gas constant.
For the volume after compression, we assume: V
f = 1 cm^3 = 1e-6 m^3
Next, we have to decide on the formula. Realistically the result will be somewhere between isothermal and adiabatic compression. As we have no timeframe given, let's assume much of the heat can radiate away during the process and hence approximate with isothermal compression.
Hence the formula we wish to use is
W = nRT*ln(Vf/Vi).
We know everything except n already.
The constant n can be calculate via the ideal gas law: PV = nRT, which one can rewrite to PV/(RT) = n. We want to use our initial constants to calculate, so we set P=P
i and V=V
i.
n = P
iV
i/(RT) = 101325 * 1.08321*10^21 /(8.31446261815324 *287.15) = 4.5971245199524130154748212636626018e22 mol
With that we can set into our work equation:
W = nRT*ln(V
f/V
i) = 4.5971245199524130154748212636626018e22 * 8.31446261815324 * 287.15 * ln(1e-6 / (1.08321*10^21) ) = -6.8322967317565033689058904003415604549381658604763144197894522284e27 J
The minus signifies that work is done on the object in this case (as the formula is for the work the gas does). So that would be our solution.
However, I see one immediate problem here. This is less than the work gravity would do for is (the change in GBE). That basically indicates that this approximation is too garbage to use. At least, unless I have made a mistake. Maybe some more high-end assumptions would be justified...